96 research outputs found
Tidally induced warps of spiral galaxies in IllustrisTNG
Abstract Warps are common features in both stellar and gaseous discs of nearby spiral galaxies with the latter usually easier to detect. Several theories have been proposed in the literature to explain their formation and prevalence, including tidal interactions with external galaxies. Observational correlations also suggest the importance of tides for warp formation. Here, we use the TNG100 run from the magnetohydrodynamical cosmological simulation suite IllustrisTNG to investigate the connection between interactions and the formation of gas warps. We find that in the sample of well-resolved gas-rich spiral galaxies (1010 ≲ M*/M⊙ ≲ 1011 at z = 0) from the simulation TNG100-1, about 16% possess the characteristic S-shaped warp. Around one-third of these objects have their warps induced by interactions with other galaxies. Half of these interactions end with the perturber absorbed by the host by z = 0. We find that warps induced by interactions survive on average for <1 Gyr, similarly to the remaining S-shaped warps. The angle between the orbital angular momentum of the perturber and the angular momentum of the host’s disc that most likely leads to warp formation is around 45 degrees. While our main goal is to investigate tidally induced warps, we find that during interactions in addition to tides, new gas that is accreted from infalling satellites also can contribute to warp formation
Always on the tipping point : A search for signals of past societies and related peatland ecosystem critical transitions during the last 6500 years in Poland
The research was funded by a grant from the National Science Centre (Poland) (No 2015/17/B/ST10/01656). The work was also made in the framework of the National Programme of Development of Humanities project (No 2bH15015483) as well as budgetary sources for scientific activity in 2016–2019, project number 0342/IP1/2016/74. V.E.J.J. was supported by the French National Research Agency (MIXOPEAT project, grant number ANR-17-CE01–0007). We thank Julie Loisel help with the calculation of the peat carbon accumulation rates. We thank also Jerzy Sikora and Paweł Zawilski for defining the chronology of the potsherd found during field surveys in the Głęboczek vicinity, and Sambor Czerwiński for constructing the lidar terrain map of the study area.Peer reviewedPublisher PD
Study of the Sextans dwarf spheroidal galaxy from the DART CaII triplet survey
We use VLT/FLAMES intermediate resolution (R~6500) spectra of individual red
giant branch stars in the near-infrared CaII triplet (CaT) region to
investigate the wide-area metallicity properties and internal kinematics of the
Sextans dwarf spheroidal galaxy (dSph). Our final sample consists of 174
probable members of Sextans with accurate line-of-sight velocities (+- 2 km/s)
and CaT [Fe/H] measurements (+- 0.2 dex). We use the MgI line at 8806.8 \AA\,
as an empirical discriminator for distinguishing between probable members of
the dSph (giant stars) and probable Galactic contaminants (dwarf stars).
Sextans shows a similar chemo-dynamical behaviour to other Milky Way dSphs,
with its central regions being more metal rich than the outer parts and with
the more metal-rich stars displaying colder kinematics than the more metal-poor
stars. Hints of a velocity gradient are found along the projected major axis
and along an axis at P.A.=191 deg, however a larger and more spatially extended
sample may be necessary to pin down the amplitude and direction of this
gradient. We detect a cold kinematic substructure at the centre of Sextans,
consistent with being the remnant of a disrupted very metal poor stellar
cluster. We derive the most extended line-of-sight velocity dispersion profile
for Sextans, out to a projected radius of 1.6 deg. From Jeans modelling of the
observed line-of-sight velocity dispersion profile we find that this is
consistent with both a cored dark matter halo with large core radius and cuspy
halo with low concentration. The mass within the last measured point is in the
range 2-4 x 10^8 M_sun, giving very large mass-to-light ratios, from 460 to 920
(M/L)_(V,sun).Comment: 30 pages, 17 figures; 4 tables. Accepted for publication in MNRAS.
Table 4 will appear as online material in the published version of the
manuscript. Typo correcte
Discrepant Mass Estimates in the Cluster of Galaxies Abell 1689
We present a new mass estimate of a well-studied gravitational lensing
cluster, Abell 1689, from deep Chandra observations with a total exposure of
200 ks. Within r=200 h-1 kpc, the X-ray mass estimate is systematically lower
than that of lensing by 30-50%. At r>200 h-1 kpc, the mass density profiles
from X-ray and weak lensing methods give consistent results. The most recent
weak lensing work suggest a steeper profile than what is found from the X-ray
analysis, while still in agreement with the mass at large radii. Previous
studies have suggested that cooler small-scale structures can bias X-ray
temperature measurements or that the northern part of the cluster is disturbed.
We find these scenarios unlikely to resolve the central mass discrepancy since
the former requires 70-90% of the space to be occupied by these cool structures
and excluding the northern substructure does not significantly affect the total
mass profiles. A more plausible explanation is a projection effect. We also
find that the previously reported high hard-band to broad-band temperature
ratio in A1689, and many other clusters observed with Chandra, may be resulting
from the instrumental absorption that decreases 10-15% of the effective area at
~1.75 keV.Comment: 18 pages, 15 figures. ApJ accepte
The X-ray Cluster Normalization of the Matter Power Spectrum
The number density of galaxy clusters provides tight statistical constraints
on the matter fluctuation power spectrum normalization, traditionally phrased
in terms of sigma_8, the root mean square mass fluctuation in spheres with
radius 8 h^-1 Mpc. We present constraints on sigma_8 and the total matter
density Omega_m0 from local cluster counts as a function of X-ray temperature,
taking care to incorporate and minimize systematic errors that plagued previous
work with this method. In particular, we present new determinations of the
cluster luminosity - temperature and mass - temperature relations, including
their intrinsic scatter, and a determination of the Jenkins mass function
parameters for the same mass definition as the mass - temperature calibration.
Marginalizing over the 12 uninteresting parameters associated with this method,
we find that the local cluster temperature function implies sigma_8
(Omega_m0/0.32)^alpha = 0.86+/-0.04 with alpha = 0.30 (0.41) for Omega_m0 <
0.32 (Omega_mo > 0.32) (68% confidence for two parameters). This result agrees
with a wide range of recent independent determinations, and we find no evidence
of any additional sources of systematic error for the X-ray cluster temperature
function determination of the matter power spectrum normalization. The joint
WMAP5 + cluster constraints are: Omega_m0 = 0.30+0.03/-0.02 and sigma_8 =
0.85+0.04/-0.02 (68% confidence for two parameters).Comment: 31 pages, 16 figures, accept for publication in ApJ 609, Jan. 10,
200
Diffuse light and building history of the galaxy cluster Abell 2667
We have searched for diffuse intracluster light in the galaxy cluster Abell
2667 (z=0.233) from HST images in three filters. We have applied to these
images an iterative multi-scale wavelet analysis and reconstruction technique,
which allows to subtract stars and galaxies from the original images. We detect
a zone of diffuse emission south west of the cluster center (DS1), and a second
faint object (ComDif), within DS1. Another diffuse source (DS2) may be
detected, at lower confidence level, north east of the center. These sources of
diffuse light contribute to 10-15% of the total visible light in the cluster.
Whether they are independent entities or are part of the very elliptical
external envelope of the central galaxy remains unclear. VLT VIMOS integral
field spectroscopy reveals a faint continuum at the positions of DS1 and ComDif
but do not allow to compute a redshift. A hierarchical substructure detection
method reveals the presence of several galaxy pairs and groups defining a
similar direction as the one drawn by the DS1-central galaxy-DS2 axis. The
analysis of archive XMM-Newton and Chandra observations shows X-ray emission
elongated in the same direction. The X-ray temperature map shows the presence
of a cool core, a broad cool zone stretching from north to south and hotter
regions towards the north east, south west and north west. This possibly
suggests shock fronts along these directions produced by infalling material.
These various data are consistent with a picture in which diffuse sources are
concentrations of tidal debris and harassed matter expelled from infalling
galaxies by tidal stripping and undergoing an accretion process onto the
central cluster galaxy; as such, they are expected to be found along the main
infall directions.Comment: Accepted for publication in Astronomy and Astrophysic
The ACS LCID project. VI. The SFH of the Tucana dSph and the relative ages of the isolated dSph galaxies
We present a detailed study of the star formation history (SFH) of the Tucana
dwarf spheroidal galaxy. High quality, deep HST/ACS data, allowed us to obtain
the deepest color-magnitude diagram to date, reaching the old main sequence
turnoff (F814 ~ 29) with good photometric accuracy. Our analysis, based on
three different SFH codes, shows that Tucana is an old and metal-poor stellar
system, which experienced a strong initial burst of star formation at a very
early epoch (~ 13 Gyr ago) which lasted a maximum of 1 Gyr (sigma value). We
are not able to unambiguously answer the question of whether most star
formation in Tucana occurred before or after the end of the reionization era,
and we analyze alternative scenarios that may explain the transformation of
Tucana from a gas-rich galaxy into a dSph. Current measurements of its radial
velocity do not preclude that Tucana may have crossed the inner regions of the
Local Group once, and so gas stripping by ram pressure and tides due to a close
interaction cannot be ruled out. On the other hand, the high star formation
rate measured at early times may have injected enough energy into the
interstellar medium to blow out a significant fraction of the initial gas
content. Gas that is heated but not blown out would also be more easily
stripped via ram pressure. We compare the SFH inferred for Tucana with that of
Cetus, the other isolated LG dSph galaxy in the LCID sample. We show that the
formation time of the bulk of star formation in Cetus is clearly delayed with
respect to that of Tucana. This reinforces the conclusion of Monelli et al.
(2010) that Cetus formed the vast majority of its stars after the end of the
reionization era implying, therefore, that small dwarf galaxies are not
necessarily strongly affected by reionization, in agreement with many
state-of-the-art cosmological models. [abridged]Comment: Accepted for publication on ApJ, 19 pages, 10 figures, 2 tables. A
version with full resolution figures is available at
http://www.iac.es/project/LCID/?p=publication
Prospects for a Dark Matter annihilation signal towards the Sagittarius dwarf galaxy with ground based Cherenkov telescopes
Dwarf galaxies are widely believed to be among the best targets for indirect
dark matter searches using high-energy gamma rays; and indeed gamma-ray
emission from these objects has long been a subject of detailed study for
ground-based atmospheric Cherenkov telescopes. Here, we update current
exclusion limits obtained on the closest dwarf, the Sagittarius dwarf galaxy,
in light of recent realistic dark matter halo models. The constraints on the
velocity-weighted annihilation cross section of the dark matter particle are of
a few 10 cms in the TeV energy range for a 50 h exposure.
The limits are extrapolated to the sensitivities of future Cherenkov Telescope
Arrays. For 200 h of observation time, the sensitivity at 95% C.L. reaches
10 cms. Possible astrophysical backgrounds from gamma-ray
sources dissembled in Sagittarius dwarf are studied. It is shown that with
long-enough observation times, gamma-ray background from millisecond pulsars in
a globular cluster contained within Sagittarius dwarf may limit the sensitivity
to dark matter annihilations.Comment: 12 pages, 5 figures, 2 tables, accepted for publication in Ap
The Star Formation & Chemical Evolution History of the Fornax Dwarf Spheroidal Galaxy
We present deep photometry in the B,V and I filters from CTIO/MOSAIC for
about 270.000 stars in the Fornax dwarf Spheroidal galaxy, out to a radius of
r_ell\sim0.8 degrees. By combining the accurately calibrated photometry with
the spectroscopic metallicity distributions of individual Red Giant Branch
stars we obtain the detailed star formation and chemical evolution history of
Fornax. Fornax is dominated by intermediate age (1-10 Gyr) stellar populations,
but also includes ancient (10-14 Gyr), and young (<1 Gyr) stars. We show that
Fornax displays a radial age gradient, with younger, more metal-rich
populations dominating the central region. This confirms results from previous
works. Within an elliptical radius of 0.8 degrees, or 1.9 kpc from the centre,
a total mass in stars of 4.3x10^7 Msun was formed, from the earliest times
until 250 Myr ago. Using the detailed star formation history, age estimates are
determined for individual stars on the upper RGB, for which spectroscopic
abundances are available, giving an age-metallicity relation of the Fornax dSph
from individual stars. This shows that the average metallicity of Fornax went
up rapidly from [Fe/H]<-2.5 dex to [Fe/H]=-1.5 dex between 8-12 Gyr ago, after
which a more gradual enrichment resulted in a narrow, well-defined sequence
which reaches [Fe/H]\sim-0.8 dex, \sim3 Gyr ago. These ages also allow us to
measure the build-up of chemical elements as a function of time, and thus
determine detailed timescales for the evolution of individual chemical
elements. A rapid decrease in [Mg/Fe] is seen for the stars with [Fe/H]>-1.5
dex, with a clear trend in age.Comment: 18 pages, 20 figure
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